Session 7 of Course 2 (Point Commutators

Strings exist in space. This space contains waves and scattered wave residue in various regions that it exists. Space where there are no waves or wave residue is said to be non-kinematic. Kinematic space, on the other hand, is the eigenset of space-time-fabric. Space-Time-Favric is the integration of all things in the continuum that ever change as operators. Yet non-kinematic space is often an operand for phenomena that pair thru its regions. In this picture, not everything is a summation of many strings. Strings form the identity of phenomena that form the basis of energy. Kinetic energy, matter, and electromagnetic energy are the "movers and the shakers" of things that change in the Continuum. Yet, these phenomena are by far mostly empty space. The rudimentary cause of how the basic phenomena that cause change in our Continuum based on our global perspective is one that shows that these must be a group of phenomena that are greater in number than strings that allow strings to exist persist, and differentiate. This idea leads to the idea of point commutators. A string momentarily exists in a spot. When it is detected, it has iterated and reiterated in a similar spot many times, changing its position and orientation based on its convergence upon the locus that it devolves upon within that region of the Continuum. What is observed as a string is a series iteration of a phenomena that keeps coming back to a relative locus. Now, if that string is what it is based on in the general solution, then what is to become of it in-between iterations, and what gives that string the ability to go all of the way around the Continuum many times within a very brief metric while still allowing that string to encode for the same phenomenon while yet being basically the same? The answer is simple. The string hermitianly breaks down into stuff after it is iterated. Stuff in-between the strings brings the strings around the Continuum. This stuff, via wave complimentation and supplementation, causes the strings to encode the same and to come back to the same general spot as the same general thing, and this set of phenomena is a group of many groups of point particles that form in-between where strings form.

Point Commutators can do this because these have totally different norm conditions than strings. Strings and their Fock Spaces form rectangular segments, while point commutators form with one point being normal to the plane of another set of points of a similar nature. The different nature of a point commutator is that these points are less than half full of condensed oscillation. Strings are only half full of condensed oscillation. The Fock Space of point commutators are always more than half empty. Yet always, Fock Space contains more free wave oscillation (not condensed) in the direct field of its neighborhood. Such a point as a point commutator may be a member of a semigroup whose differential geometry pulls dissociated string material around the Continuum while sharing condensed wave oscillation in such a way as to stabilize the jointal conditions of the dissociated strings by supplementing the tangential spurs of any wave propagation that is rooted at the center states of the points (allowing the radial functions of the points to be maintained). Such stabilization works to maintain the encodement of the points so as to form the string that is at the locus that it must be at.